We have observed the diatomic $nsns\ensuremath{\rightarrow}ns(n+1)s\ensuremath{\rightarrow}(n+1)s(n+1)s$ microwave transitions of pairs of cold Rb Rydberg atoms for $36<n<48$ . The $ns(n+1)s$ state has by far the largest van der Waals shift due to its near degeneracy with the nearby $n{p}_{3/2}n{p}_{3/2}$ state. In fact, the energy difference and the van der Waals shift change sign at $n=38$ and we observe shifts of both signs. The combined excitation of the $ns(n+1)s$ and $(n+1)s(n+1)s$ states leads to an unusual line shape which can be described by a three-level Floquet model.We have observed the diatomic $nsns\ensuremath{\rightarrow}ns(n+1)s\ensuremath{\rightarrow}(n+1)s(n+1)s$ microwave transitions of pairs of cold Rb Rydberg atoms for $36<n<48$. The $ns(n+1)s$ state has by far the largest van der Waals shift due to its near degeneracy with the nearby $n{p}_{3/2}n{p}_{3/2}$ state. In fact, the energy difference and the van der Waals shift change sign at $n=38$ and we observe shifts of both signs. The combined excitation of the $ns(n+1)s$ and $(n+1)s(n+1)s$ states leads to an unusual line shape which can be described by a three-level Floquet model.

Physical Review AMay 12, 200934 citations

We have observed the diatomic $nsns\ensuremath{\rightarrow}ns(n+1)s\ensuremath{\rightarrow}(n+1)s(n+1)s$ microwave transitions of pairs of cold Rb Rydberg atoms for

36<n<48

. The

ns(n+1)s

state has by far the largest van der Waals shift due to its near degeneracy with the nearby

n{p}_{3/2}n{p}_{3/2}

state. In fact, the energy difference and the van der Waals shift change sign at

n=38

and we observe shifts of both signs. The combined excitation of the

ns(n+1)s

and

(n+1)s(n+1)s

states leads to an unusual line shape which can be described by a three-level Floquet model.